Objects of the §5.3 additive energy estimate e.left.to.show #
Source: enhance.tex 8271–8882. The matrix field
F(t,x) = ∑_{k∈2ℤ+1} ξ_{m,k}(t) (I + ∇Χ_{m,k}) ∘ X⁻¹_{m-1,l_k}(t,x) (8298–8302), the leading
term F ∇T_{m-1} of e.leadingord, the space average ⟨FᵗF⟩(t) of e.ergodic.break.up, and
the material gradient D_{t,m-1} ∇T_{m-1} of e.barf.cascade.
Conventions: gradMatrix Χ x has entry (i,j) = ∂_{x_i} χ_{e_j} (e.gradcorrmatrix), so the
leading term is the matrix–vector product F.mulVec (∇T).
F(t,x) := ∑_{k∈2ℤ+1} ξ_{m,k}(t) (I + ∇Χ_{m,k}(t,·)) ∘ X⁻¹_{m-1,l_k}(t,x) (source 8298–8302),
with κm = κ_m the diffusivity of the correctors. For each t only finitely many summands are
nonzero (xiMK_odd_support_finite).
Equations
- One or more equations did not get rendered due to their size.
Instances For
The leading-order gradient F ∇T_{m-1} of e.leadingord / e.left.to.show.
Equations
- AVenhance.Infra.Section5.LeftToShow.leadingGrad I hΦ m κm T t x = (AVenhance.Infra.Section5.LeftToShow.leadingMatrix I hΦ m κm t x).mulVec (AVenhance.spaceGrad (T t) x)
Instances For
The space average ⟨FᵗF⟩(t) of e.ergodic.break.up / e.bracket.FF.
Equations
- One or more equations did not get rendered due to their size.
Instances For
The material gradient D_t ∇T = (∂_t + b·∇)∇T, componentwise (e.D.t.m.def,
e.barf.cascade with b = b_{m-1}).
Equations
- AVenhance.Infra.Section5.LeftToShow.materialGrad b T t x i = AVenhance.Infra.Section5.materialDerivative (fun (s : ℝ) (y : Homogenization.Vec 2) => AVenhance.spaceGrad (T s) y i) b t x